In classical theory, a physical state is an equivalence class under ga
uge transformations. Is the same true in quantum theory? The physical
quantum states are the solutions of Dirac's quantum constraint equatio
n. They cannot be constructed as equivalence classes under the ''simpl
e'' gauge transformations generated by the Dirac constraints. However,
we show here that they can be constructed as equivalence classes unde
r suitably defined ''complete'' gauge transformations. The complete ga
uge transformations are generated by the action of the quantum constra
ints on arbitrary individual components of the state.